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Spectromicroscopy

Welcome

The beamline houses unique microscope designed for studies of the local band structure of the materials. VUV beam is focused into a sub-µm spot and electrons arising from the photoemission process are collected and analyzed in terms of their angular and energy distributions (ARPES). Thanks to the beam focusing the photoelectron spectrum is acquired as a function of its origin on a sample surface coordinate system. The final focusing is performed with one of the two Schwarzschild objectives designed for 27 and 74 eV of photon energy. The ARPES is performed with energy and angular resolutions down to 14 meV and 0.150by means of internal movable electron energy analyzer mounted on precision two axes goniometer setup . The sample can be measured at 15-470 K and the sample focusing and imaging are performed thanks to the XYZR sampe scanning stage.Read more...

Charge carrier anisotropic motion in twisted few-layer graphene

The dependence of the interlayer coupling on the twist angle is analyzed and, in the domains with tri-layers and more, if different rotations are present, the electrons in weaker coupled adjacent layers are shown to have different properties manifested by coexisting van Hove singularities, moiré superlattices with corresponding superlattice Dirac points, and charge carrier group velocity renormalizations. V. Kandyba et al. Sci. Rep. 5, 16388 (2015).

Comparing Graphene Growth on Cu(111) versus Oxidized Cu(111)

The growth on copper oxide, a high-k dielectric material, preserves the intrinsic properties of graphene; it is not doped and a linear dispersion is observed close to the Fermi energy.
S. Gottardi et al, Nano Lett. 2015, 15, 917.

Spin–orbit coupling in the band structure of monolayer WSe2

We used angle-resolved photoemission spectroscopy (ARPES) to map out the band structure of single-layer WSe2. The splitting of the top of the valence band because of spin–orbit coupling is 513 ± 10 meV, in general agreement with theoretical predictions and in the same range as that of bulk WSe2. Duy Lee et al, J. Phys.: Cond. Matter 2015.

ARPES on graphene domains grown on industrially relevant substrates

A real space map of graphene grain orientation on the copper foil visualized through photoemission microscopy with integrated intensity from around the Dirac point of a specific orientation. The two colors, red and blue, correspond to signal from two different graphene orientations.N. Wilson et al, Nano Research 6, 99-112, (2013)

A microscopic view on the metal-insulator transition in a Mott system

We unveil for the first time the metal-insulator transition (MIT) in Cr-doped V2O3 with submicron lateral resolution: with decreasing temperature, microscopic domains become metallic and coexist with an insulating background.

News

April 2018

Congratulations to prof. Takeshi Kondo and colleagues for publishing their paper "A weak topological insulator state in quasi-one-dimensional bismuth iodide" in Nature. The contribution of Elettra was monitoring periodicity of band dispersions on topologically dark and topologically non trivial facets of Bi4I4 needles thanks to high photon flux at sub-μm focus of Spectromicroscopy beamline.

April 2016

Congratulations to our collaborators Duy Le, Edwin Preciado, Miguel Isarraraz, Iori Tanabe, Takashi Komesu, Conrad Troha, Ludwig Bartels, Talat S Rahman and Peter A Dowben, whose paper has been highlighted among the best papers of 2015 in JPCM! (Nanostructures & nanoelectronics)
The selection is done on the basis of reviewers' opinions as well as on the number of total downloads within the year and about 25 papers from 1800 candidates are so selected.

User Area

We invite users and collaborators to discuss their proposals with the beamline local contactsin advance before the submission deadline. This may be crucial for a careful assessment of the experiment feasibility and may result in an improvement of the proposal. Please read carefully guidelines for proposal rating-submission.More info.

Call for proposals

The deadline for proposal submission for beamtime allocation from January 1st to June 30th, 2019 will be September 17th, 2018.